Coming to MXenes, magnetism is mostly realized in bare surface cases due to unpaired \(d\) -electrons [1]}, [2]}. With the presence of surface groups, the \(M(d)\) -orbitals form covalent bonding with the \(T(p)\) -orbitals and as a result the magnetism disappears (e.g. in \(Ti_2CO_2\)  , \(Ti_2CF_2\)  and \(Ti_2C(OH)_2)\) ). However, there are exceptions: \(Cr\) -based carbides and nitrides are predicted to show magnetism with terminated surface groups (\(T = O\) , \(OH\) , or \(F\) ) up to nearly room temperature [1]}, [2]}. The present work is mainly on examining the intrinsic anomalous Hall effect (AHE) that occurs in ferro(i)magnetic systems driven by spin-orbit interaction. In this regard, the anomalous and ordinary Hall contributions are known to be proportional to the magnetization (M) and applied magnetic field (H) respectively [5]}, [6]}. This is in fact another reason to explore anomalous Hall effect in nitride MXenes rather than carbides as \(^{\prime }N^{\prime }\)  has one extra electron compared to \(^{\prime }C^{\prime }\)  [7]}. In any case, to the best of our knowledge, no such experimental or theoretical efforts have ever been made earlier in these intrinsic 2D magnets with a focus on AHE.
